WO2018008070A1 - Inspecting device and method - Google Patents
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- WO2018008070A1 WO2018008070A1 PCT/JP2016/069816 JP2016069816W WO2018008070A1 WO 2018008070 A1 WO2018008070 A1 WO 2018008070A1 JP 2016069816 W JP2016069816 W JP 2016069816W WO 2018008070 A1 WO2018008070 A1 WO 2018008070A1
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- electromagnetic wave
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- bias voltage
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- terahertz wave
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
- G01N21/3581—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light using far infrared light; using Terahertz radiation
Definitions
- the present invention relates to a technical field of an inspection apparatus and method for inspecting a subject using electromagnetic waves.
- this type of device for example, it has asymmetric forward and reverse current-voltage characteristics, operates as an oscillating element at a first operating point that exhibits negative differential resistance, and exhibits nonlinear characteristics that are not in the negative resistance region.
- An apparatus including an oscillation detection element that operates as a detection element at two operating points has been proposed (see Patent Document 1).
- Patent Document 1 has temperature dependence and has some individual differences. For this reason, unless the bias voltage applied to the element is appropriately set according to the use environment of the element, it may be difficult to maintain the stability of the detection operation. However, Patent Document 1 does not disclose how to set the bias voltage.
- the present invention has been made in view of the above problems, for example, and an object of the present invention is to provide an inspection apparatus and method capable of realizing a stable detection operation.
- the inspection apparatus of the present invention irradiates a subject with an electromagnetic wave generation unit, an electromagnetic wave detection unit, a reflection unit that can reflect an electromagnetic wave, and an electromagnetic wave generated from the electromagnetic wave generation unit During a part of the inspection period, the electromagnetic wave is incident on the electromagnetic wave detection unit without passing through the subject by the reflection unit, and is applied to the electromagnetic wave detection unit based on the detection sensitivity of the electromagnetic wave detection unit Adjusting means for adjusting the bias voltage to be applied.
- an inspection method of the present invention is an inspection method in an inspection apparatus including an electromagnetic wave generation unit, an electromagnetic wave detection unit, and a reflection unit capable of reflecting an electromagnetic wave, from the electromagnetic wave generation unit
- the electromagnetic wave is incident on the electromagnetic wave detection unit by the reflection unit without passing through the test object during a part of the examination period in which the generated electromagnetic wave is irradiated on the test object, and the electromagnetic wave detection unit detects the electromagnetic wave.
- An adjustment step of adjusting a bias voltage applied to the electromagnetic wave detection unit based on sensitivity is provided.
- the inspection apparatus includes an electromagnetic wave generation unit, an electromagnetic wave detection unit, and an adjustment unit that adjusts a bias voltage applied to the electromagnetic wave detection unit.
- the adjusting means includes: a reflection part capable of reflecting electromagnetic waves; and a part of the examination period in which the electromagnetic wave generated from the electromagnetic wave generation part is irradiated on the subject without causing the reflection part to pass through the subject. Then, the light is incident on the electromagnetic wave detection unit, and the bias voltage is adjusted based on the detection sensitivity of the electromagnetic wave detection unit.
- An example of the electromagnetic wave is a terahertz wave.
- the bias voltage is adjusted based on the detection sensitivity of the electromagnetic wave detection unit during a part of the inspection period (that is, during the inspection period). For example, even when the optimum value of the bias voltage changes due to a temperature change during the inspection period, the inspection apparatus can apply the optimum bias voltage to the electromagnetic wave detection unit. Therefore, according to the inspection apparatus, a stable detection operation can be realized.
- the reflection unit is provided at least at a part of the periphery of the placement unit on which the subject is placed.
- the inspection apparatus further includes a scanning unit that moves the electromagnetic wave generation unit and the electromagnetic wave detection unit integrally so that the subject and the reflection unit are irradiated with the electromagnetic wave during the inspection period.
- the reflection unit is disposed on the optical path of the electromagnetic wave connecting the electromagnetic wave generation unit and the subject.
- the inspection apparatus reflects the reflection part so that the electromagnetic wave is incident on the electromagnetic wave detection part without passing through the subject during a part of the inspection period, and the subject is irradiated with the electromagnetic wave in the other part of the inspection period.
- Angle changing means for changing the angle of the surface with respect to the electromagnetic wave is further provided.
- the bias voltage can be adjusted relatively easily during a part of the inspection period.
- the electromagnetic wave detection unit includes an electromagnetic wave detection element having nonlinearity in current-voltage characteristics.
- the adjustment means sequentially changes the voltage value of the bias voltage applied to the electromagnetic wave detection unit (that is, applied to the electromagnetic wave detection element) during a part of the inspection period, so that the detection sensitivity of the electromagnetic wave detection unit is maximized.
- the bias voltage is adjusted to a voltage value lower than the specified voltage value by a predetermined value.
- the electromagnetic wave detection element may be a resonant tunnel diode. According to this aspect, it is possible to suitably detect a terahertz wave as an example of an electromagnetic wave.
- the inspection method is an inspection method in an inspection apparatus including an electromagnetic wave generation unit, an electromagnetic wave detection unit, and a reflection unit capable of reflecting electromagnetic waves.
- the electromagnetic wave is incident on the electromagnetic wave detection unit without passing through the subject by the reflection unit during a part of the inspection period in which the electromagnetic wave generated from the electromagnetic wave generation unit is irradiated on the subject.
- An adjustment step of adjusting a bias voltage applied to the electromagnetic wave detection unit based on the detection sensitivity of the electromagnetic wave detection unit is provided.
- a stable detection operation can be realized as in the inspection apparatus according to the above-described embodiment.
- various aspects similar to the various aspects of the inspection apparatus according to the embodiment described above can be employed.
- a terahertz wave measuring apparatus is taken as an example of an inspection apparatus according to the present invention.
- a terahertz wave is mentioned as an example of the electromagnetic wave which concerns on this invention.
- FIG. 1 is a schematic configuration diagram illustrating the configuration of the terahertz wave measuring apparatus according to the first embodiment.
- FIG. 2 is a conceptual diagram illustrating a measurement operation of the terahertz wave measuring apparatus according to the first embodiment.
- the terahertz wave measuring apparatus 1 includes an imaging head unit 10, a signal processing / control unit 20, a bias voltage generation unit 21, a signal amplifier 22, and a scanning mechanism 23.
- the terahertz wave measuring device 1 is a so-called flat bed type device (see FIG. 2A).
- the terahertz wave measuring apparatus 1 includes a sample stage 32 made of, for example, a fluororesin for placing the measurement object 90 and a scanner cover 33 that covers the measurement object 90.
- the imaging head unit 10 includes a generation unit 11, a collimating lens 12, a beam splitter 13, an objective lens 14, a condenser lens 15, and a detection unit 16.
- the generating unit 11 includes a terahertz wave generating element 11a and a horn antenna 11b.
- the detection unit 16 includes a terahertz wave detection element 16a and a horn antenna 16b.
- a bias voltage generated by the bias voltage generation unit 21 is applied to each of the terahertz wave generating element 11a and the terahertz wave detecting element 16a.
- a bias voltage modulated based on a predetermined reference signal is applied to the terahertz wave generating element 11a.
- the terahertz wave modulated at a constant frequency is emitted from the generation unit 11.
- the terahertz wave emitted from the generator 11 is applied to the measurement object 90 through the collimator lens 12, the beam splitter 13, the objective lens 14, and the sample stage 32.
- the terahertz wave reflected by the measurement object 90 enters the detection unit 16 via the sample stage 32, the objective lens 14, the beam splitter 13, and the condenser lens 15. From the detection unit 16, a reception signal corresponding to the incident terahertz wave is output.
- the scanning mechanism 23 drives the imaging head unit 10 based on the drive signal from the signal processing / control unit 20. Specifically, as shown in FIG. 2B, a so-called raster scan is performed by the scan mechanism 23. The scanning mechanism 23 further generates an imaging position signal for monitoring the irradiation position of the terahertz wave emitted from the imaging head unit 10.
- the signal processing / control unit 20 receives the reception signal output from the detection unit 16 via the signal amplifier 22.
- the signal processing / control unit 20 uses the terahertz wave reception data signal generated from the reception signal output from the detection unit 16 and the scan mechanism 23.
- a mapped terahertz wave image is generated based on the generated imaging position signal. It should be noted that various existing aspects can be applied to the method for generating a terahertz wave image image, and therefore, detailed description thereof is omitted.
- the terahertz wave measuring apparatus 1 includes a terahertz wave for reflecting the terahertz wave emitted from the generating unit 11 around the sample stage 32 and inside the housing 31 (that is, on the imaging head unit 10 side).
- a reflector 34 is provided.
- the imaging head unit 10 and the terahertz wave reflecting unit 34 are overlapped when viewed in plan from above the terahertz wave measuring apparatus 1.
- the imaging head unit 10 is driven.
- the imaging head unit 10 and the terahertz wave reflection unit 34 overlap that is, when the imaging head 10 is positioned below the terahertz wave reflection unit 34
- the terahertz wave emitted from the generation unit 11 is the measurement object 90. Without being irradiated, is reflected by the terahertz wave reflection unit 34 and enters the detection unit 16.
- a resonant tunnel diode (Resonant Tunneling Diode: RTD) is used as the terahertz wave detecting element 16a.
- RTD Resonant Tunneling Diode
- the resonant tunnel diode as the terahertz wave detecting element 16a will be described with reference to FIG.
- the resonant tunneling diode has a differential negative resistance region showing differential negative resistance characteristics in the current-voltage characteristics of its operating region (see the range from point B to point C in FIG. 3).
- the resonant tunneling diode further has a non-linear region exhibiting strong non-linear characteristics in the vicinity of the differential negative resistance region (see the range from point A to point B in FIG. 3).
- the resonant tunneling diode functions as a terahertz wave generating element when a bias voltage corresponding to the differential negative resistance region is applied.
- the resonant tunneling diode functions as a terahertz detecting element when a bias voltage corresponding to the nonlinear region is applied.
- the non-linear region is limited to a relatively narrow voltage range
- the resonant tunneling diode in order for the resonant tunneling diode to operate stably as a terahertz wave detecting element, it is necessary to control the bias voltage with high accuracy. For this reason, if the bias voltage changes, or if the optimum bias voltage of the resonant tunneling diode changes due to, for example, a temperature change, the detection sensitivity may be significantly reduced (details will be described later).
- the bias voltage of the terahertz wave detecting element 16a is set (or calibrated).
- the setting process of the bias voltage of the terahertz wave detection element 16a will be described with reference mainly to the flowchart of FIG.
- the signal processing / control unit 20 determines whether the imaging head unit 10 is located below the terahertz wave reflection unit 34 based on the imaging position signal generated by the scanning mechanism 23. (Step S101). In this determination, when it is determined that the imaging head unit 10 is not located below the terahertz wave reflection unit 34 (step S101: No), the signal processing / control unit 20 performs the process of step S101 again. That is, the imaging head unit 10 is in a standby state until it is positioned below the terahertz wave reflection unit 34.
- step S101 when it is determined in step S101 that the imaging head unit 10 is located below the terahertz wave reflection unit 34 (step S101: Yes), the signal processing / control unit 20 applies the terahertz wave detection element 16a.
- the bias voltage generation unit 21 is controlled so as to initialize the bias voltage to be executed (step S102).
- the signal processing / control unit 20 controls the bias voltage generation unit 21 so that the bias voltage applied to the terahertz wave detection element 16a is increased by a predetermined value ⁇ V1 from the current value (step S103).
- the signal processing / control unit 20 detects the signal amplitude of the reception signal output from the detection unit 16 (that is, the terahertz wave detection element 16a) (step S104).
- the signal processing / control unit 20 compares the signal amplitude detected last time with the signal amplitude detected this time, and determines whether or not the signal amplitude has decreased (step S105).
- the signal amplitude corresponds to the detection sensitivity of the terahertz wave detection element 16a.
- the detection sensitivity of the terahertz wave detection element 16a will be described with reference to FIG. Note that points A and B in FIG. 5 correspond to points A and B in FIG. As can be seen from FIG. 5, the detection sensitivity of the resonant tunneling diode as the terahertz wave detection element 16a increases as the bias voltage increases. However, when the bias voltage exceeds the voltage corresponding to point B (that is, the voltage at which the detection sensitivity is maximized), the detection sensitivity of the resonant tunneling diode is rapidly lost. That is, the resonant tunneling diode does not function as a terahertz wave detecting element.
- step S105 when the signal amplitude is reduced” in the determination in step S105 means a case where the bias voltage applied to the terahertz wave detection element 16a exceeds the voltage at which the detection sensitivity is maximized.
- step S105: No the signal processing / control unit 20 performs the process of step S103.
- the initial value of the signal amplitude detected last time may be set to zero, for example.
- step S105 determines whether the signal amplitude has decreased (step S105: Yes). If it is determined in step S105 that the signal amplitude has decreased (step S105: Yes), the signal processing / control unit 20 performs bias so that the bias voltage is reduced by a predetermined value ⁇ V2 from the current value.
- the voltage generator 21 is controlled (step S106).
- the significance of reducing the bias voltage by a predetermined value ⁇ V2 from the current value will be described with reference to FIG.
- a voltage corresponding to point B in FIG. 5 is applied as a bias voltage to the terahertz wave detection element 16a
- the detection sensitivity of the terahertz wave detection element 16a can be maximized.
- the bias voltage fluctuates during measurement of the measurement object 90, for example, the resonant tunnel diode may not function as the terahertz wave detection element 16a.
- the bias voltage is lower than the voltage at which the detection sensitivity is maximized (the voltage corresponding to the range from point D to point E in FIG. 5) by a predetermined value ⁇ V2.
- the bias voltage is reduced.
- the predetermined value ⁇ V1 may be appropriately set in consideration of, for example, the time required for the bias voltage setting process, the voltage error of the bias voltage generation unit 21, and the like.
- the predetermined value ⁇ V2 may be appropriately set in consideration of, for example, the predetermined value ⁇ V1 and the voltage-detection sensitivity characteristic related to the terahertz wave detection element 16a.
- the above-described bias voltage setting process is repeated.
- the bias voltage is reset (or calibrated) every time the imaging head unit 10 is positioned below the terahertz wave reflection unit 34. For this reason, an optimal bias voltage can always be applied to the terahertz wave detecting element 16a, and the stable measurement operation of the terahertz wave measuring apparatus 1 can be realized.
- the “terahertz wave generating element 11a”, the “terahertz wave detecting element 16a”, the “terahertz wave reflecting unit 34”, the “signal processing / control unit 20”, and the “measurement object 90” according to the present embodiment are each represented by the present invention. Is an example of “electromagnetic wave generation unit”, “electromagnetic wave detection unit”, “reflection unit”, “adjusting means”, and “subject”.
- the generation unit 11 may include a plurality of terahertz wave generation elements 11a and horn antennas 11b arranged in an array.
- the detection unit 16 may include a plurality of terahertz wave detection elements 16a and horn antennas 16b arranged in an array.
- a hemispherical or super hemispherical silicon lens may be used instead of the beam splitter 13, for example, a half mirror, a combination of a polarizer and a quarter wavelength plate, or the like can be applied.
- FIGS. 6 to 8 A second embodiment of the terahertz wave measuring apparatus will be described with reference to FIGS.
- the second embodiment is the same as the first embodiment described above except that the configuration of the terahertz wave measuring apparatus and part of the bias voltage setting process are different. Therefore, in the second embodiment, the description overlapping with that of the first embodiment is omitted, and the common portions in the drawing are denoted by the same reference numerals and only FIGS. 6 to 8 are basically different only. The description will be given with reference.
- FIG. 6 is a schematic configuration diagram illustrating the configuration of the terahertz wave measuring apparatus according to the second embodiment.
- FIG. 7 is a conceptual diagram showing the measurement operation of the terahertz wave measuring apparatus according to the second embodiment.
- the terahertz wave measuring apparatus 2 includes an imaging head unit 10 ′, a signal processing / control unit 20, a bias voltage generation unit 21, a signal amplifier 22, a polygon mirror driving unit 24, a polygon mirror 41, and an objective lens 42. It is configured.
- the polygon mirror 41 when the measurement target 90 is measured, the polygon mirror 41 is rotated by the polygon mirror drive unit 24, so that the terahertz wave emitted from the generation unit 11 scans the measurement target 90 (see FIG. 7).
- the reflection surface of the polygon mirror 41 faces the imaging head unit 10 ′ during a part of the period, so that the terahertz wave emitted from the generation unit 11 is measured.
- the object 90 is not irradiated, but is reflected by the polygon mirror 41 and enters the detector 16 (see FIG. 7D).
- the bias voltage of the terahertz wave detection element 16a is set (or calibrated) based on the reception signal output from the detection unit 16.
- the setting process of the bias voltage of the terahertz wave detection element 16a will be described with reference to the flowchart of FIG.
- the signal processing / control unit 20 stores the current bias voltage as the memory 1 (that is, the value of the variable “memory 1” relating to the bias voltage is set as the current bias voltage) (step S201). ).
- the signal processing / control unit 20 refers to, for example, the drive signal of the polygon mirror drive unit 24 to determine whether or not the polygon mirror 41 faces the imaging head unit 10 ′ (that is, emitted from the generation unit 11). Whether the incident angle of the terahertz wave with respect to the reflection surface of the polygon mirror 41 is 0 degree or not is determined (step S202).
- step S202 If it is determined in step S202 that the polygon mirror 41 does not face the imaging head unit 10 '(step S202: No), the signal processing / control unit 20 performs the process of step S202 again. During the period until the polygon mirror 41 faces the imaging head unit 10 ′, the measurement object 90 is measured.
- step S202 when it is determined in step S202 that the polygon mirror 41 is directly facing the imaging head unit 10 '(step S202: Yes), the signal processing / control unit 20 is applied to the terahertz wave detection element 16a.
- the bias voltage generator 21 is controlled so as to initialize the bias voltage to be initialized (step S203).
- the signal processing / control unit 20 controls the bias voltage generation unit 21 so that the bias voltage applied to the terahertz wave detection element 16a is increased by a predetermined value ⁇ V1 from the current value (step S204).
- the signal processing / control unit 20 determines whether or not the polygon mirror 41 is facing the imaging head unit 10 '(step S205). In this determination, when it is determined that the polygon mirror 41 is directly facing the imaging head unit 10 ′ (step S205: Yes), the signal processing / control unit 20 detects the detection unit 16 (that is, the terahertz wave detection element 16a). The signal amplitude of the received signal output from is detected (step S206).
- the signal processing / control unit 20 compares the signal amplitude detected last time with the signal amplitude detected this time, and determines whether or not the signal amplitude has decreased (step S207). In this determination, when it is determined that the signal amplitude has not decreased (step S207: No), the signal processing / control unit 20 performs the process of step S204.
- step S207 determines whether the signal amplitude has decreased. If it is determined in step S207 that the signal amplitude has decreased (step S207: Yes), the signal processing / control unit 20 performs bias so that the bias voltage is reduced from the current value by a predetermined value ⁇ V2. The voltage generator 21 is controlled (step S208).
- step S205 If it is determined in step S205 that the polygon mirror 41 does not face the imaging head unit 10 '(step S205: No), the signal processing / control unit 20 stores the current bias voltage as the memory 2. (That is, the value of the variable “memory 2” relating to the bias voltage is set as the current bias voltage) (step S209).
- the signal processing / control unit 20 controls the bias voltage generation unit 21 so that the bias voltage returns to the value recorded in the memory 1 (step S210).
- the terahertz wave emitted from the generation unit 11 is irradiated to the measurement object 90.
- the measurement of the measurement object 90 is appropriately performed.
- the signal processing / control unit 20 determines whether or not the polygon mirror 41 is facing the imaging head unit 10 '(step S211). In this determination, when it is determined that the polygon mirror 41 does not face the imaging head unit 10 ′ (step S211: No), the signal processing / control unit 20 performs the process of step S211 again. During the period until the polygon mirror 41 faces the imaging head unit 10 ′, the measurement object 90 is measured.
- step S211 If it is determined in step S211 that the polygon mirror 41 is directly facing the imaging head unit 10 '(step S211: Yes), the signal processing / control unit 20 has the bias voltage recorded in the memory 2.
- the bias voltage generation unit 21 is controlled so as to be a value (step S212), and the process of step S206 is performed.
- the “polygon mirror 41” according to the present embodiment is another example of the “reflecting portion” according to the present invention.
- the “polygon mirror drive unit 24” according to the present embodiment is an example of the “angle changing unit” according to the present invention.
- the polygon mirror 41 is not limited to a quadrangle (see FIG. 6).
- the objective lens 42 for example, an f- ⁇ lens may be used.
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Abstract
Description
本発明は、電磁波を用いて被検体を検査する検査装置及び方法の技術分野に関する。 The present invention relates to a technical field of an inspection apparatus and method for inspecting a subject using electromagnetic waves.
この種の装置として、例えば、非対称の順方向及び逆方向電流電圧特性を有し、負性微分抵抗を示す第1動作点で発振素子として動作し、負性抵抗領域ではない非線形特性を示す第2動作点で検出素子として動作する発振検出素子を備える装置が提案されている(特許文献1参照)。 As this type of device, for example, it has asymmetric forward and reverse current-voltage characteristics, operates as an oscillating element at a first operating point that exhibits negative differential resistance, and exhibits nonlinear characteristics that are not in the negative resistance region. An apparatus including an oscillation detection element that operates as a detection element at two operating points has been proposed (see Patent Document 1).
特許文献1に記載の発振検出素子は、温度依存性を有しており、また多少の個体差もある。このため、素子の使用環境に応じて該素子に印加されるバイアス電圧を適宜設定しなければ、検出動作の安定性を保つことが困難になる可能性がある。しかしながら、特許文献1には、バイアス電圧をどのように設定するかは開示されていない。
The oscillation detection element described in
本発明は、例えば上記問題点に鑑みてなされたものであり、安定した検出動作を実現することができる検査装置及び方法を提供することを課題とする。 The present invention has been made in view of the above problems, for example, and an object of the present invention is to provide an inspection apparatus and method capable of realizing a stable detection operation.
本発明の検査装置は、上記課題を解決するために、電磁波発生部と、電磁波検出部と、電磁波を反射可能な反射部と、前記電磁波発生部から発生された電磁波が被検体に照射される検査期間の一部の期間に、前記電磁波を、前記反射部により前記被検体を介さずに、前記電磁波検出部に入射させ、前記電磁波検出部の検出感度に基づいて、前記電磁波検出部に印加されるバイアス電圧を調整する調整手段と、を備える。 In order to solve the above problems, the inspection apparatus of the present invention irradiates a subject with an electromagnetic wave generation unit, an electromagnetic wave detection unit, a reflection unit that can reflect an electromagnetic wave, and an electromagnetic wave generated from the electromagnetic wave generation unit During a part of the inspection period, the electromagnetic wave is incident on the electromagnetic wave detection unit without passing through the subject by the reflection unit, and is applied to the electromagnetic wave detection unit based on the detection sensitivity of the electromagnetic wave detection unit Adjusting means for adjusting the bias voltage to be applied.
本発明の検査方法は、上記課題を解決するために、電磁波発生部と、電磁波検出部と、電磁波を反射可能な反射部と、を備える検査装置における検査方法であって、前記電磁波発生部から発生された電磁波が被検体に照射される検査期間の一部の期間に、前記電磁波を、前記反射部により前記被検体を介さずに、前記電磁波検出部に入射させ、前記電磁波検出部の検出感度に基づいて、前記電磁波検出部に印加されるバイアス電圧を調整する調整工程を備える。 In order to solve the above problems, an inspection method of the present invention is an inspection method in an inspection apparatus including an electromagnetic wave generation unit, an electromagnetic wave detection unit, and a reflection unit capable of reflecting an electromagnetic wave, from the electromagnetic wave generation unit The electromagnetic wave is incident on the electromagnetic wave detection unit by the reflection unit without passing through the test object during a part of the examination period in which the generated electromagnetic wave is irradiated on the test object, and the electromagnetic wave detection unit detects the electromagnetic wave. An adjustment step of adjusting a bias voltage applied to the electromagnetic wave detection unit based on sensitivity is provided.
本発明の作用及び他の利得は次に説明する実施するための形態から明らかにされる。 The operation and other advantages of the present invention will be clarified from the embodiments to be described below.
本発明の検査装置及び方法に係る実施形態について説明する。 Embodiments according to the inspection apparatus and method of the present invention will be described.
(検査装置)
実施形態に係る検査装置は、電磁波発生部と、電磁波検出部と、該電磁波検出部に印加されるバイアス電圧を調整する調整手段と、を備える。該調整手段は、電磁波を反射可能な反射部と、電磁波発生部から発生された電磁波が被検体に照射される検査期間の一部の期間に、電磁波を、反射部により被検体を介さずに、電磁波検出部に入射させ、電磁波検出部の検出感度に基づいて、バイアス電圧を調整する。電磁波の一例としては、テラヘルツ波が挙げられる。
(Inspection equipment)
The inspection apparatus according to the embodiment includes an electromagnetic wave generation unit, an electromagnetic wave detection unit, and an adjustment unit that adjusts a bias voltage applied to the electromagnetic wave detection unit. The adjusting means includes: a reflection part capable of reflecting electromagnetic waves; and a part of the examination period in which the electromagnetic wave generated from the electromagnetic wave generation part is irradiated on the subject without causing the reflection part to pass through the subject. Then, the light is incident on the electromagnetic wave detection unit, and the bias voltage is adjusted based on the detection sensitivity of the electromagnetic wave detection unit. An example of the electromagnetic wave is a terahertz wave.
当該検査装置では、検査期間の一部の期間に(即ち、検査期間中に)、電磁波検出部の検出感度に基づいてバイアス電圧が調整される。例えば検査期間中の温度変化に起因して、バイアス電圧の最適値が変化した場合であっても、当該検査装置では、電磁波検出部に最適なバイアス電圧を印加することができる。従って、当該検査装置によれば、安定した検出動作を実現することができる。 In the inspection apparatus, the bias voltage is adjusted based on the detection sensitivity of the electromagnetic wave detection unit during a part of the inspection period (that is, during the inspection period). For example, even when the optimum value of the bias voltage changes due to a temperature change during the inspection period, the inspection apparatus can apply the optimum bias voltage to the electromagnetic wave detection unit. Therefore, according to the inspection apparatus, a stable detection operation can be realized.
実施形態に係る検査装置の一態様では、反射部は、被検体が載置される載置部の周囲の少なくとも一部に設けられている。当該検査装置は、検査期間に、被検体及び反射部に電磁波が照射されるように、電磁波発生部及び電磁波検出部を一体として移動させる走査手段を更に備える。 In one aspect of the inspection apparatus according to the embodiment, the reflection unit is provided at least at a part of the periphery of the placement unit on which the subject is placed. The inspection apparatus further includes a scanning unit that moves the electromagnetic wave generation unit and the electromagnetic wave detection unit integrally so that the subject and the reflection unit are irradiated with the electromagnetic wave during the inspection period.
或いは、実施形態に係る検査装置の他の態様では、反射部は、電磁波発生部及び被検体を結ぶ電磁波の光路上に配置されている。当該検査装置は、検査期間の一部の期間に電磁波が被検体を介さずに電磁波検出部に入射し、検査期間の他の期間に電磁波が被検体に照射されるように、反射部の反射面の電磁波に対する角度を変更する角度変更手段を更に備える。 Alternatively, in another aspect of the inspection apparatus according to the embodiment, the reflection unit is disposed on the optical path of the electromagnetic wave connecting the electromagnetic wave generation unit and the subject. The inspection apparatus reflects the reflection part so that the electromagnetic wave is incident on the electromagnetic wave detection part without passing through the subject during a part of the inspection period, and the subject is irradiated with the electromagnetic wave in the other part of the inspection period. Angle changing means for changing the angle of the surface with respect to the electromagnetic wave is further provided.
これらの態様によれば、比較的容易にして、検査期間の一部の期間にバイアス電圧の調整を行うことができる。 According to these aspects, the bias voltage can be adjusted relatively easily during a part of the inspection period.
実施形態に係る検査装置の他の態様では、電磁波検出部は、電流電圧特性に非線形性を有する電磁波検出素子を含む。調整手段は、検査期間の一部の期間に、電磁波検出部に印加される(即ち、電磁波検出素子に印加される)バイアス電圧の電圧値を順次変更して、電磁波検出部の検出感度が最大となる電圧値を特定し、該特定された電圧値より所定値だけ低い電圧値に、バイアス電圧を調整する。ここで、電磁波検出素子は、共鳴トンネルダイオードであってよい。この態様によれば、電磁波の一例としてのテラヘルツ波を好適に検出することができる。 In another aspect of the inspection apparatus according to the embodiment, the electromagnetic wave detection unit includes an electromagnetic wave detection element having nonlinearity in current-voltage characteristics. The adjustment means sequentially changes the voltage value of the bias voltage applied to the electromagnetic wave detection unit (that is, applied to the electromagnetic wave detection element) during a part of the inspection period, so that the detection sensitivity of the electromagnetic wave detection unit is maximized. And the bias voltage is adjusted to a voltage value lower than the specified voltage value by a predetermined value. Here, the electromagnetic wave detection element may be a resonant tunnel diode. According to this aspect, it is possible to suitably detect a terahertz wave as an example of an electromagnetic wave.
(検査方法)
実施形態に係る検査方法は、電磁波発生部と、電磁波検出部と、電磁波を反射可能な反射部と、を備える検査装置における検査方法である。当該検査方法は、電磁波発生部から発生された電磁波が被検体に照射される検査期間の一部の期間に、電磁波を、反射部により被検体を介さずに、電磁波検出部に入射させ、該電磁波検出部の検出感度に基づいて、電磁波検出部に印加されるバイアス電圧を調整する調整工程を備える。
(Inspection method)
The inspection method according to the embodiment is an inspection method in an inspection apparatus including an electromagnetic wave generation unit, an electromagnetic wave detection unit, and a reflection unit capable of reflecting electromagnetic waves. In the inspection method, the electromagnetic wave is incident on the electromagnetic wave detection unit without passing through the subject by the reflection unit during a part of the inspection period in which the electromagnetic wave generated from the electromagnetic wave generation unit is irradiated on the subject. An adjustment step of adjusting a bias voltage applied to the electromagnetic wave detection unit based on the detection sensitivity of the electromagnetic wave detection unit is provided.
当該検査方法によれば、上述した実施形態に係る検査装置と同様に、安定した検出動作を実現することができる。尚、当該検査方法においても、上述した実施形態に係る検査装置の各種態様と同様の各種態様を採ることができる。 According to the inspection method, a stable detection operation can be realized as in the inspection apparatus according to the above-described embodiment. In the inspection method, various aspects similar to the various aspects of the inspection apparatus according to the embodiment described above can be employed.
本発明の検査装置に係る実施例について図面を参照して説明する。以下の実施例では、本発明に係る検査装置の一例として、テラヘルツ波計測装置を挙げる。また、本発明に係る電磁波の一例として、テラヘルツ波を挙げる。 Embodiments according to the inspection apparatus of the present invention will be described with reference to the drawings. In the following embodiments, a terahertz wave measuring apparatus is taken as an example of an inspection apparatus according to the present invention. Moreover, a terahertz wave is mentioned as an example of the electromagnetic wave which concerns on this invention.
<第1実施例>
テラヘルツ波計測装置の第1実施例について、図1乃至図5を参照して説明する。
<First embodiment>
A first embodiment of a terahertz wave measuring apparatus will be described with reference to FIGS.
(装置構成)
テラヘルツ波計測装置1の構成について図1及び図2を参照して説明する。図1は、第1実施例に係るテラヘルツ波計測装置の構成を示す概略構成図である。図2は、第1実施例に係るテラヘルツ波計測装置の測定動作を示す概念図である。
(Device configuration)
A configuration of the terahertz
図1において、テラヘルツ波計測装置1は、撮像ヘッド部10、信号処理・制御部20、バイアス電圧生成部21、信号増幅器22及びスキャン機構23を備えて構成されている。テラヘルツ波計測装置1は、所謂フラットベッド型の装置である(図2(a)参照)。テラヘルツ波計測装置1は、測定対象物90を載置するための、例えばフッ素樹脂等により構成された試料台32と、測定対象90を覆うスキャナカバー33とを有している。
1, the terahertz
撮像ヘッド部10は、発生部11、コリメートレンズ12、ビームスプリッタ13、対物レンズ14、集光レンズ15及び検出部16を備えて構成されている。発生部11は、テラヘルツ波発生素子11a及びホーンアンテナ11bを備えて構成されている。検出部16は、テラヘルツ波検出素子16a及びホーンアンテナ16bを備えて構成されている。
The
テラヘルツ波発生素子11a及びテラヘルツ波検出素子16a各々には、バイアス電圧生成部21により生成されるバイアス電圧が印加されている。テラヘルツ波発生素子11aには、所定の参照信号に基づいて変調されたバイアス電圧が印加される。この結果、発生部11からは、一定の周波数で変調されたテラヘルツ波が出射される。
A bias voltage generated by the bias
発生部11から出射されたテラヘルツ波は、コリメートレンズ12、ビームスプリッタ13、対物レンズ14及び試料台32を介して、測定対象物90に照射される。該測定対象物90により反射されたテラヘルツ波は、試料台32、対物レンズ14、ビームスプリッタ13及び集光レンズ15を介して、検出部16に入射する。検出部16からは、入射したテラヘルツ波に応じた受信信号が出力される。
The terahertz wave emitted from the
スキャン機構23は、信号処理・制御部20からの駆動信号に基づいて、撮像ヘッド部10を駆動する。具体的には図2(b)に示すように、スキャン機構23により、所謂ラスタースキャンが行われる。スキャン機構23は、更に、撮像ヘッド部10から照射されるテラヘルツ波の照射位置をモニタするための撮像位置信号を生成する。
The
信号処理・制御部20は、検出部16から出力された受信信号を、信号増幅器22を介して受信する。測定対象物90が当該テラヘルツ波計測装置1により測定される際は、信号処理・制御部20は、検出部16から出力された受信信号から生成されたテラヘルツ波受信データ信号と、スキャン機構23により生成された撮像位置信号とに基づいて、マッピングされたテラヘルツ波イメージ画像を生成する。尚、テラヘルツ波イメージ画像の生成方法には、既存の各種態様を適用可能であるので、その詳細についての説明は割愛する。
The signal processing /
本実施例では特に、テラヘルツ波計測装置1は、試料台32の周囲且つ筺体31の内側(即ち、撮像ヘッド部10側)に、発生部11から出射されたテラヘルツ波を反射するためのテラヘルツ波反射部34が設けられている。
Particularly in the present embodiment, the terahertz
テラヘルツ波計測装置1の動作時には、図2(b)に示すように、当該テラヘルツ波計測装置1の上方から平面的に見て、撮像ヘッド部10とテラヘルツ波反射部34とが重なるように、撮像ヘッド部10が駆動される。撮像ヘッド部10とテラヘルツ波反射部34とが重なる場合(即ち、撮像ヘッド10が、テラヘルツ波反射部34の下方に位置する場合)、発生部11から出射されたテラヘルツ波は、測定対象物90には照射されずに、テラヘルツ波反射部34で反射され検出部16に入射する。
When the terahertz
当該テラヘルツ波計測装置1では、テラヘルツ波検出素子16aとして、共鳴トンネルダイオード(Resonant Tunneling Diode:RTD)が用いられている。ここで、テラヘルツ波検出素子16aとしての共鳴トンネルダイオードについて、図3を参照して説明を加える。
In the terahertz
共鳴トンネルダイオードは、その動作領域の電流電圧特性に、微分負性抵抗特性を示す微分負性抵抗領域を有する(図3の、点B~点Cの範囲参照)。共鳴トンネルダイオードは、更に、微分負性抵抗領域付近で強い非線形特性を示す非線形領域を有する(図3の、点A~点Bの範囲参照)。 The resonant tunneling diode has a differential negative resistance region showing differential negative resistance characteristics in the current-voltage characteristics of its operating region (see the range from point B to point C in FIG. 3). The resonant tunneling diode further has a non-linear region exhibiting strong non-linear characteristics in the vicinity of the differential negative resistance region (see the range from point A to point B in FIG. 3).
共鳴トンネルダイオードは、微分負性抵抗領域に該当するバイアス電圧が印加された際に、テラヘルツ波発生素子として機能する。他方で、共鳴トンネルダイオードは、非線形領域に該当するバイアス電圧が印加された際に、テラヘルツ検出素子として機能する。 The resonant tunneling diode functions as a terahertz wave generating element when a bias voltage corresponding to the differential negative resistance region is applied. On the other hand, the resonant tunneling diode functions as a terahertz detecting element when a bias voltage corresponding to the nonlinear region is applied.
図3からわかるように、非線形領域は、比較的狭い電圧範囲に限られるため、共鳴トンネルダイオードがテラヘルツ波検出素子として安定して動作するためには、精度良くバイアス電圧を制御する必要がある。このため、仮に、バイアス電圧が変化すると、又は、例えば温度変化に起因して共鳴トンネルダイオードの最適バイアス電圧が変化すると、検出感度が著しく低下する可能性がある(詳細については後述する)。 As can be seen from FIG. 3, since the non-linear region is limited to a relatively narrow voltage range, in order for the resonant tunneling diode to operate stably as a terahertz wave detecting element, it is necessary to control the bias voltage with high accuracy. For this reason, if the bias voltage changes, or if the optimum bias voltage of the resonant tunneling diode changes due to, for example, a temperature change, the detection sensitivity may be significantly reduced (details will be described later).
そこで本実施例では、測定対象物90の測定期間の一部の期間(即ち、撮像ヘッド部10とテラヘルツ波反射部34とが重なる期間)に、検出部16から出力される受信信号に基づいて、テラヘルツ波検出素子16aのバイアス電圧の設定(又は校正)が行われる。以下、テラヘルツ波検出素子16aのバイアス電圧の設定処理について、図4のフローチャートを主に参照して説明する。
Therefore, in this embodiment, based on the reception signal output from the
(バイアス電圧の設定処理)
図4において、先ず、信号処理・制御部20は、スキャン機構23により生成された撮像位置信号に基づいて、撮像ヘッド部10が、テラヘルツ波反射部34の下方に位置するか否かを判定する(ステップS101)。この判定において、撮像ヘッド部10が、テラヘルツ波反射部34の下方に位置しないと判定された場合(ステップS101:No)、信号処理・制御部20は、再びステップS101の処理を行う。つまり、撮像ヘッド部10が、テラヘルツ波反射部34の下方に位置するまで待機状態となる。
(Bias voltage setting process)
In FIG. 4, first, the signal processing /
他方、ステップS101の判定において、撮像ヘッド部10が、テラヘルツ波反射部34の下方に位置すると判定された場合(ステップS101:Yes)、信号処理・制御部20は、テラヘルツ波検出素子16aに印加されるバイアス電圧を初期化するように、バイアス電圧生成部21を制御する(ステップS102)。
On the other hand, when it is determined in step S101 that the
次に、信号処理・制御部20は、テラヘルツ波検出素子16aに印加されるバイアス電圧を、現在値から所定値ΔV1だけ増加するように、バイアス電圧生成部21を制御する(ステップS103)。このとき、信号処理・制御部20は、検出部16(即ち、テラヘルツ波検出素子16a)から出力された受信信号の信号振幅を検出する(ステップS104)。
Next, the signal processing /
次に、信号処理・制御部20は、前回検出された信号振幅と今回検出された信号振幅とを比較して、信号振幅が低下したか否かを判定する(ステップS105)。ここで、信号振幅は、テラヘルツ波検出素子16aの検出感度に相当する。
Next, the signal processing /
テラヘルツ波検出素子16aの検出感度について、図5を参照して説明を加える。尚、図5における点A及び点Bは、図3における点A及び点Bに対応している。図5からわかるように、テラヘルツ波検出素子16aとしての共鳴トンネルダイオードの検出感度は、バイアス電圧が高くなるにつれて高くなる。しかしながら、バイアス電圧が、点Bに相当する電圧(つまり、検出感度が最大となる電圧)を超えると、共鳴トンネルダイオードの検出感度は急激に失われる。即ち、共鳴トンネルダイオードは、テラヘルツ波検出素子として機能しなくなる。
The detection sensitivity of the terahertz
従って、ステップS105の判定における「信号振幅が低下した場合」とは、テラヘルツ波検出素子16aに印加されたバイアス電圧が、検出感度が最大となる電圧を超えた場合を意味する
ステップS105の判定において、信号振幅が低下していないと判定された場合(ステップS105:No)、信号処理・制御部20は、ステップS103の処理を行う。尚、前回検出された信号振幅の初期値は、例えばゼロ等とすればよい。このように構成すれば、ステップS102の処理によりバイアス電圧が初期化された後、初めてステップS105の判定が行われる場合も、「S105:No」と進み、ステップS103の処理が行われる。
Therefore, “when the signal amplitude is reduced” in the determination in step S105 means a case where the bias voltage applied to the terahertz
他方、ステップS105の判定において、信号振幅が低下したと判定された場合(ステップS105:Yes)、信号処理・制御部20は、バイアス電圧を、現在値から所定値ΔV2だけ小さくするように、バイアス電圧生成部21を制御する(ステップS106)。
On the other hand, if it is determined in step S105 that the signal amplitude has decreased (step S105: Yes), the signal processing /
ここで、バイアス電圧を、現在値から所定値ΔV2だけ小さくする意義について、図5を参照して説明を加える。理想的には、図5における点Bに相当する電圧がバイアス電圧として、テラヘルツ波検出素子16aに印加されれば、該テラヘルツ波検出素子16aの検出感度を最大とすることができる。しかしながら、測定対象物90の測定中に、例えばバイアス電圧が変動した場合、共鳴トンネルダイオードがテラヘルツ波検出素子16aとして機能しなくなる可能性がある。
Here, the significance of reducing the bias voltage by a predetermined value ΔV2 from the current value will be described with reference to FIG. Ideally, if a voltage corresponding to point B in FIG. 5 is applied as a bias voltage to the terahertz
そこで本実施例では、バイアス電圧が、検出感度が最大となる電圧よりも低い電圧(図5の、点D~点Eの範囲に相当する電圧)となるように、現在値から所定値ΔV2だけバイアス電圧を小さくするのである。このように構成すれば、テラヘルツ波検出素子16aの動作の安定性と、良好な検出感度との両立を図ることができる。
Therefore, in this embodiment, the bias voltage is lower than the voltage at which the detection sensitivity is maximized (the voltage corresponding to the range from point D to point E in FIG. 5) by a predetermined value ΔV2. The bias voltage is reduced. With this configuration, it is possible to achieve both the stability of the operation of the terahertz
所定値ΔV1は、例えば、当該バイアス電圧の設定処理にかかる時間や、バイアス電圧生成部21の電圧誤差等を考慮して適宜設定すればよい。所定値ΔV2は、例えば、所定値ΔV1や、テラヘルツ波検出素子16aに係る電圧-検出感度特性等を考慮して適宜設定すればよい。
The predetermined value ΔV1 may be appropriately set in consideration of, for example, the time required for the bias voltage setting process, the voltage error of the bias
(技術的効果)
本実施例では、上述したバイアス電圧の設定処理が繰り返し行われる。この結果、撮像ヘッド部10がテラヘルツ波反射部34の下方に位置する度に、バイアス電圧が再設定(又は校正)される。このため、テラヘルツ波検出素子16aに、常に最適なバイアス電圧を印加することができ、当該テラヘルツ波計測装置1の安定した測定動作を実現することができる。
(Technical effect)
In this embodiment, the above-described bias voltage setting process is repeated. As a result, the bias voltage is reset (or calibrated) every time the
本実施例に係る「テラヘルツ波発生素子11a」、「テラヘルツ波検出素子16a」、「テラヘルツ波反射部34」、「信号処理・制御部20」及び「測定対象物90」は、夫々、本発明に係る「電磁波発生部」、「電磁波検出部」、「反射部」、「調整手段」及び「被検体」の一例である。
The “terahertz
尚、発生部11は、テラヘルツ波発生素子11a及びホーンアンテナ11bが複数個アレイ状に配列されていてよい。同様に、検出部16も、テラヘルツ波検出素子16a及びホーンアンテナ16bが複数個アレイ状に配列されていてよい。また、ホーンアンテナに代えて、半球状や超半球状のシリコンレンズが用いられてもよい。ビームスプリッタ13に代えて、例えばハーフミラーや、偏光子及び1/4波長板の組合せ、等を適用可能である。
The
<第2実施例>
テラヘルツ波計測装置の第2実施例について、図6乃至図8を参照して説明する。第2実施例では、テラヘルツ波計測装置の構成及びバイアス電圧の設定処理の一部が異なっている以外は、上述した第1実施例と同様である。よって、第2実施例について、第1実施例と重複する説明を省略すると共に、図面上における共通箇所には同一符号を付して示し、基本的に異なる点についてのみ、図6乃至図8を参照して説明する。
<Second embodiment>
A second embodiment of the terahertz wave measuring apparatus will be described with reference to FIGS. The second embodiment is the same as the first embodiment described above except that the configuration of the terahertz wave measuring apparatus and part of the bias voltage setting process are different. Therefore, in the second embodiment, the description overlapping with that of the first embodiment is omitted, and the common portions in the drawing are denoted by the same reference numerals and only FIGS. 6 to 8 are basically different only. The description will be given with reference.
(装置構成)
テラヘルツ波計測装置2の構成について図6及び図7を参照して説明する。図6は、第2実施例に係るテラヘルツ波計測装置の構成を示す概略構成図である。図7は、第2実施例に係るテラヘルツ波計測装置の測定動作を示す概念図である。
(Device configuration)
The configuration of the terahertz
図6において、テラヘルツ波計測装置2は、撮像ヘッド部10´、信号処理・制御部20、バイアス電圧生成部21、信号増幅器22、ポリゴンミラー駆動部24、ポリゴンミラー41及び対物レンズ42を備えて構成されている。
6, the terahertz
本実施例では、測定対象物90の測定時に、ポリゴンミラー駆動部24によりポリゴンミラー41が回転駆動されることによって、発生部11から出射されたテラヘルツ波が、測定対象物90を走査する(図7参照)。
In this embodiment, when the
図7からわかるように、ポリゴンミラー41が回転すると、一部の期間では、ポリゴンミラー41の反射面が撮像ヘッド部10´と正対するため、発生部11から出射されたテラヘルツ波が、測定対象物90には照射されずに、ポリゴンミラー41で反射され検出部16に入射する(図7(d)参照)。
As can be seen from FIG. 7, when the
本実施例では、測定対象物90の測定期間の一部の期間(即ち、発生部11から出射されたテラヘルツ波が、ポリゴンミラー41により反射され、測定対象物90に照射されずに、検出部16に入射する期間)に、検出部16から出力される受信信号に基づいて、テラヘルツ波検出素子16aのバイアス電圧の設定(又は校正)が行われる。以下、テラヘルツ波検出素子16aのバイアス電圧の設定処理について、図8のフローチャートを参照して説明する。
In the present embodiment, a part of the measurement period of the measurement object 90 (that is, the terahertz wave emitted from the
(バイアス電圧の設定処理)
図8において、先ず、信号処理・制御部20は、現在のバイアス電圧をメモリ1として記憶する(即ち、バイアス電圧に係る変数「メモリ1」の値を、現在のバイアス電圧とする)(ステップS201)。
(Bias voltage setting process)
In FIG. 8, first, the signal processing /
次に、信号処理・制御部20は、例えばポリゴンミラー駆動部24の駆動信号を参照して、ポリゴンミラー41が撮像ヘッド部10´に正対しているか否か(即ち、発生部11から出射されたテラヘルツ波の、ポリゴンミラー41の反射面に対する入射角が0度であるか否か)を判定する(ステップS202)。
Next, the signal processing /
ステップS202の判定において、ポリゴンミラー41が撮像ヘッド部10´に正対していないと判定された場合(ステップS202:No)、信号処理・制御部20は、再びステップS202の処理を行う。ポリゴンミラー41が撮像ヘッド部10´に正対するまでの期間は、測定対象物90の測定が行われる。
If it is determined in step S202 that the
他方、ステップS202の判定において、ポリゴンミラー41が撮像ヘッド部10´に正対していると判定された場合(ステップS202:Yes)、信号処理・制御部20は、テラヘルツ波検出素子16aに印加されるバイアス電圧を初期化するように、バイアス電圧生成部21を制御する(ステップS203)。
On the other hand, when it is determined in step S202 that the
次に、信号処理・制御部20は、テラヘルツ波検出素子16aに印加されるバイアス電圧を、現在値から所定値ΔV1だけ増加するように、バイアス電圧生成部21を制御する(ステップS204)。
Next, the signal processing /
次に、信号処理・制御部20は、ポリゴンミラー41が撮像ヘッド部10´に正対しているか否かを判定する(ステップS205)。この判定において、ポリゴンミラー41が撮像ヘッド部10´に正対していると判定された場合(ステップS205:Yes)、信号処理・制御部20は、検出部16(即ち、テラヘルツ波検出素子16a)から出力された受信信号の信号振幅を検出する(ステップS206)。
Next, the signal processing /
次に、信号処理・制御部20は、前回検出された信号振幅と今回検出された信号振幅とを比較して、信号振幅が低下したか否かを判定する(ステップS207)。この判定において、信号振幅が低下していないと判定された場合(ステップS207:No)、信号処理・制御部20は、ステップS204の処理を行う。
Next, the signal processing /
他方、ステップS207の判定において、信号振幅が低下したと判定された場合(ステップS207:Yes)、信号処理・制御部20は、バイアス電圧を、現在値から所定値ΔV2だけ小さくするように、バイアス電圧生成部21を制御する(ステップS208)。
On the other hand, if it is determined in step S207 that the signal amplitude has decreased (step S207: Yes), the signal processing /
ステップS205の判定において、ポリゴンミラー41が撮像ヘッド部10´に正対していないと判定された場合(ステップS205:No)、信号処理・制御部20は、現在のバイアス電圧をメモリ2として記憶する(即ち、バイアス電圧に係る変数「メモリ2」の値を、現在のバイアス電圧とする)(ステップS209)。
If it is determined in step S205 that the
続いて、信号処理・制御部20は、バイアス電圧がメモリ1に記録されている値に戻るように、バイアス電圧生成部21を制御する(ステップS210)。ステップS205の判定において、ポリゴンミラー41が撮像ヘッド部10´に正対していないと判定された場合、発生部11から出射されたテラヘルツ波が測定対象物90に照射される。このとき、バイアス電圧がメモリ1に記憶されている値に戻されることによって、測定対象物90の測定が適切に行われるのである。
Subsequently, the signal processing /
次に、信号処理・制御部20は、ポリゴンミラー41が撮像ヘッド部10´に正対しているか否かを判定する(ステップS211)。この判定において、ポリゴンミラー41が撮像ヘッド部10´に正対していないと判定された場合(ステップS211:No)、信号処理・制御部20は、再びステップS211の処理を行う。ポリゴンミラー41が撮像ヘッド部10´に正対するまでの期間は、測定対象物90の測定が行われる。
Next, the signal processing /
ステップS211の判定において、ポリゴンミラー41が撮像ヘッド部10´に正対していると判定された場合(ステップS211:Yes)、信号処理・制御部20は、バイアス電圧がメモリ2に記録されている値になるように、バイアス電圧生成部21を制御して(ステップS212)、ステップS206の処理を行う。
If it is determined in step S211 that the
(技術的効果)
本実施例では、特に、原理的に発生する、ポリゴンミラー41が撮像ヘッド部10´に正対する時(即ち、発生部11から出射されたテラヘルツ波の、ポリゴンミラー41の反射面に対する入射角が0度である時)に、テラヘルツ波検出素子16aのバイアス電圧が再設定(又は校正)される。ポリゴンミラー41が撮像ヘッド部10´に正対する時は、測定期間のデッドタイムに当たるので、バイアス電圧の再設定により測定時間が延長されることはない。
(Technical effect)
In the present embodiment, in particular, when the
本実施例に係る「ポリゴンミラー41」は、本発明に係る「反射部」の他の例である。本実施例に係る「ポリゴンミラー駆動部24」は、本発明に係る「角度変更手段」の一例である。
The “
尚、ポリゴンミラー41は、四角形(図6参照)に限定されない。また、対物レンズ42には、例えばf-θレンズが用いられてよい。
The
本発明は、上述した実施形態に限られるものではなく、請求の範囲及び明細書全体から読み取れる発明の要旨或いは思想に反しない範囲で適宜変更可能であり、そのような変更を伴う検査装置及び方法もまた本発明の技術的範囲に含まれるものである。 The present invention is not limited to the above-described embodiment, and can be appropriately changed without departing from the spirit or idea of the invention that can be read from the claims and the entire specification, and an inspection apparatus and method with such a change. Is also included in the technical scope of the present invention.
1、2…テラヘルツ波計測装置、10、10´…撮像ヘッド部、11a…テラヘルツ波発生素子、16a…テラヘルツ波検出素子、20…信号処理・制御部、21…バイアス電圧生成部、22…信号増幅器、23…スキャン機構、24…ポリゴンミラー駆度部、34…反射部、41…ポリゴンミラー、90…測定対象物
DESCRIPTION OF
Claims (7)
電磁波検出部と、
電磁波を反射可能な反射部と、
前記電磁波発生部から発生された電磁波が被検体に照射される検査期間の一部の期間に、前記電磁波を、前記反射部により前記被検体を介さずに、前記電磁波検出部に入射させ、前記電磁波検出部の検出感度に基づいて、前記電磁波検出部に印加されるバイアス電圧を調整する調整手段と、
を備えることを特徴とする検査装置。 An electromagnetic wave generator,
An electromagnetic wave detection unit;
A reflective part capable of reflecting electromagnetic waves;
The electromagnetic wave generated from the electromagnetic wave generation unit is incident on the electromagnetic wave detection unit without passing through the test object by the reflection unit during a part of the examination period in which the test object is irradiated with the electromagnetic wave. An adjusting means for adjusting a bias voltage applied to the electromagnetic wave detection unit based on the detection sensitivity of the electromagnetic wave detection unit;
An inspection apparatus comprising:
前記検査期間に、前記被検体及び前記反射部に前記電磁波が照射されるように、前記電磁波発生部及び前記電磁波検出部を一体として移動させる走査手段を更に備える
ことを特徴とする請求項1に記載の検査装置。 The reflecting portion is provided at least at a part of the periphery of the placement portion on which the subject is placed;
The scanning apparatus according to claim 1, further comprising a scanning unit that moves the electromagnetic wave generation unit and the electromagnetic wave detection unit as a unit so that the electromagnetic wave is irradiated to the subject and the reflection unit during the examination period. The inspection device described.
前記一部の期間に前記電磁波が前記被検体を介さずに前記電磁波検出部に入射し、前記検査期間の他の期間に前記電磁波が前記被検体に照射されるように、前記反射部の反射面の前記電磁波に対する角度を変更する角度変更手段を更に備える
ことを特徴とする請求項1に記載の検査装置。 The reflecting portion is disposed on an optical path of the electromagnetic wave that connects the electromagnetic wave generating portion and the subject,
Reflection of the reflection unit is performed such that the electromagnetic wave is incident on the electromagnetic wave detection unit without passing through the subject during the partial period, and the electromagnetic wave is irradiated on the subject during the other period of the examination period. The inspection apparatus according to claim 1, further comprising an angle changing unit that changes an angle of the surface with respect to the electromagnetic wave.
前記調整手段は、前記一部の期間に、前記バイアス電圧の電圧値を順次変更して前記検出感度が最大となる電圧値を特定し、前記特定された電圧値より所定値だけ低い電圧値に、前記バイアス電圧を調整する
ことを特徴とする請求項1に記載の検査装置。 The electromagnetic wave detection unit includes an electromagnetic wave detection element having nonlinearity in current-voltage characteristics,
The adjusting means sequentially changes the voltage value of the bias voltage during the partial period to specify a voltage value at which the detection sensitivity is maximized, and sets the voltage value to a voltage value lower than the specified voltage value by a predetermined value. The inspection apparatus according to claim 1, wherein the bias voltage is adjusted.
前記電磁波発生部から発生された電磁波が被検体に照射される検査期間の一部の期間に、前記電磁波を、前記反射部により前記被検体を介さずに、前記電磁波検出部に入射させ、前記電磁波検出部の検出感度に基づいて、前記電磁波検出部に印加されるバイアス電圧を調整する調整工程を備える
ことを特徴とする検査方法。 An inspection method in an inspection apparatus comprising an electromagnetic wave generation unit, an electromagnetic wave detection unit, and a reflection unit capable of reflecting electromagnetic waves,
The electromagnetic wave generated from the electromagnetic wave generation unit is incident on the electromagnetic wave detection unit without passing through the test object by the reflection unit during a part of the examination period in which the test object is irradiated with the electromagnetic wave. An inspection method comprising: an adjustment step of adjusting a bias voltage applied to the electromagnetic wave detection unit based on detection sensitivity of the electromagnetic wave detection unit.
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Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2020090784A1 (en) * | 2018-10-30 | 2020-05-07 | パイオニア株式会社 | Electromagnetic-wave detecting device and electromagnetic-wave detecting system |
| EP3633333A4 (en) * | 2017-06-02 | 2021-03-10 | Pioneer Corporation | DEVICE FOR DETECTING ELECTROMAGNETIC WAVES AND METHOD FOR SETTING THE DETECTION SIGNAL ACQUISITION TIME |
| JPWO2020090783A1 (en) * | 2018-10-30 | 2021-09-24 | パイオニア株式会社 | Electromagnetic wave detection system |
| WO2024038784A1 (en) * | 2022-08-19 | 2024-02-22 | 国立大学法人大阪大学 | Signal detection device and signal detection method |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2014106127A (en) * | 2012-11-28 | 2014-06-09 | Pioneer Electronic Corp | Terahertz wave measurement instrument and method |
| JP2015087163A (en) * | 2013-10-29 | 2015-05-07 | パイオニア株式会社 | Terahertz wave measuring device |
| JP2015180047A (en) * | 2014-02-28 | 2015-10-08 | キヤノン株式会社 | element |
Family Cites Families (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH07260684A (en) * | 1994-03-28 | 1995-10-13 | Nippon Telegr & Teleph Corp <Ntt> | High-accuracy reflectance measuring method and measuring instrument |
| JP3821364B2 (en) * | 2001-10-11 | 2006-09-13 | 株式会社島津製作所 | Measurement conditions setting method for photoelectric photometry |
| JP2005321728A (en) * | 2004-05-11 | 2005-11-17 | Olympus Corp | Method for determining measurement parameter of scanning type microscope |
| DE102005045163B4 (en) * | 2005-09-21 | 2007-06-14 | Leica Microsystems Cms Gmbh | Apparatus and method for detection with a scanning microscope |
| US8362430B1 (en) * | 2007-09-05 | 2013-01-29 | Jefferson Science Assosiates, LLC | Method for large and rapid terahertz imaging |
| JP6099114B2 (en) * | 2011-06-14 | 2017-03-22 | ローム株式会社 | Wireless transmission device |
| JP2015152347A (en) * | 2014-02-12 | 2015-08-24 | 住友電気工業株式会社 | Spectroscopic analysis apparatus and spectral analysis method |
| JP6475523B2 (en) * | 2015-03-13 | 2019-02-27 | 日本信号株式会社 | Control circuit and detector |
-
2016
- 2016-07-04 WO PCT/JP2016/069816 patent/WO2018008070A1/en not_active Ceased
- 2016-07-04 JP JP2018525846A patent/JP6761471B2/en active Active
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2014106127A (en) * | 2012-11-28 | 2014-06-09 | Pioneer Electronic Corp | Terahertz wave measurement instrument and method |
| JP2015087163A (en) * | 2013-10-29 | 2015-05-07 | パイオニア株式会社 | Terahertz wave measuring device |
| JP2015180047A (en) * | 2014-02-28 | 2015-10-08 | キヤノン株式会社 | element |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP3633333A4 (en) * | 2017-06-02 | 2021-03-10 | Pioneer Corporation | DEVICE FOR DETECTING ELECTROMAGNETIC WAVES AND METHOD FOR SETTING THE DETECTION SIGNAL ACQUISITION TIME |
| WO2020090784A1 (en) * | 2018-10-30 | 2020-05-07 | パイオニア株式会社 | Electromagnetic-wave detecting device and electromagnetic-wave detecting system |
| JPWO2020090783A1 (en) * | 2018-10-30 | 2021-09-24 | パイオニア株式会社 | Electromagnetic wave detection system |
| JP2022161995A (en) * | 2018-10-30 | 2022-10-21 | パイオニア株式会社 | Electromagnetic wave detection system |
| JP2024116206A (en) * | 2018-10-30 | 2024-08-27 | パイオニア株式会社 | Electromagnetic Wave Detection System |
| WO2024038784A1 (en) * | 2022-08-19 | 2024-02-22 | 国立大学法人大阪大学 | Signal detection device and signal detection method |
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